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<strong>GRAVITY</strong>/HEAT INTERACTION APPENDIX V Let us suppose that we have to investigate the question whether gravitative action alone upon some given substance or alloy can produce heat. We do not specify its texture, density nor atomic structure. We assume simply the flux of gravitative action followed by an increase of heat in the alloy. If we assume a small circular surface on the alloy then the gravitative flux on it may be expressed by Gauss' Theorem and it is 4 n M, where M represents the mass of all sub-surface particles. The question is, can this expression be transformed into heat. We will assume it can be. Now recalling the relativity law connecting mass and energy: where: T = kinetic energy m o = initial mass c = velocity of light M = m o + T/c 2 (by Einstein) we set 4 pi M = m o +m o v 2 2c 2 But v 2 /c 2 is a proper fraction; hence M = m o + m o /2k In the boundary case v = c, then M = m o ( 1 + 1/k). For all other cases, 4 pi M = m o (k+1 ) where k =/= 0 k Strictly, M should be preceded by a conversion factor 1/k but if inserted, it does not alter the results. Thus if gravity could produce heat, the effect is limited to a narrow range, as this result shows. It merits stress that in a gravitational field the flow lines of descent are Geodesies. J. Wickenden 71
APPENDIX VI WEIGHT-MASS ANOMALY There is a great need for a precise experimental determination of the weight to mass ratio of protons or electrons. Since the ratio for a proton plus an electron is known already, the determination of the ratio for either particle is sufficient. The difficulty of a direct determination of the gravitational deflection of a charged particle in an experiment similar to the neutron or neutral atom experiment is due to electrical forces being much greater than gravitational field forces. Thus stray electrons or ions which are always present on the walls of an apparatus can exert sufficient force to completely mask the gravitational force. Even if the surface charges are neglected, image charges of the electron beam itself and self-repulsion in the beam may obscure at the gravitational deflection. An additional problem is the earth's magnetic field. Electrons of even a few volts energy will feel a force due to the earth's field a thousand billion times larger than the gravitational deflection. This last problem is avoided in a static measurement of the ratio such as a weighing of ionized matter. However, this last method has the additional difficulty of requiring a high proportion of ionized to unionized matter in the sample being weighed. Of course all these problems can be resolved to some extent but it is questionable if an experiment of either of the above types can be designed in which all the adverse effects can simultaneously be sufficiently minimized. Probably a completely new type of experiment will have to be devised to measure the weight to mass ratio of the proton or electron. Such a measurement may detect a deviation from the law of constant weight to mass ratio. If such an anomaly can be shown to exist, there is the possibility of finding a material which would be acted upon in an unusual manner in a gravitational field. Martin L. Perl* "Editor's Note: Martin L. Perl is the recipient of the 1995 Nobel Prize in physics. 72
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was highly questioned Copyright© 1
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EXPLORATION OF ANOMALOUS GRAVITY EF
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As aerospace engineers we deal more
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( DxB) ∂ fH = , (2) ∂t where D
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BREAKTHROUGH PROPULSION PHYSICS RES
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PROGRAM PRIORITIES To simultaneousl
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STATUS AND DIRECTION A government s
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REPORT DOCUMENTATION PAGE Public re
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Recent calculations have indicated
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Casimir force has only been compute
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Cavity width 125 nm Cavity wall 245
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Also shown for comparison, is the c
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AIAA-2001-3906 SEARCH FOR EFFECTS O
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AIAA-2001-3906 Experiment 2 - Time-
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AIAA-2001-3906 Resonance - 0 flow R
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AIAA-2001-3906 Einstein Rocket -- E
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Tests of Mach's Principle with a Me
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we note that Woodward [4] has made
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and their tensioning mechanism. Ele
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Conclusion The test of Mach’s pri
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velocity of the “front” that mu
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Fortunately, recent advances in non
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The time difference between two wel
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impinging at normal incident on a m
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sooner than his challenger. Interes
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non-empty space¯time with a horizo
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metric of S-1 takes the form ds 2 =
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L. Hui Astrophys. J. 519 (1999), p.
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consistent with the boundary condit
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classical behaviour is recovered fo
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Heisenberg's equations for the posi
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(2K) Fig. 1. Behaviour of Q(t) for
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5. N.A. Lemos J. Math. Phys. 37 (19
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arXiv:cond-mat/9701074 v3 16 Sep 19
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technology involved in the construc
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3 Operation of the apparatus. Two i
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following: in a field gradient of 0
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inner edge of the toroid (5-7 mm fr
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7 Discussion. The interaction of a
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8.1 Acknowledgments. The author is
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High T c materials, fabrication |ge
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Supporting solenoids |general, fig.
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Rotating solenoids |general, fig. 3
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Cryogenic system |general, fig. 51/
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Disk braking system |general, fig.
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In two recent experiments [1, 2], P
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true, must then consist of some kin
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constant turns Eintein gravity into
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[2] E. Podkletnov and A.D. Levit, G
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Proposal for the Experimental Detec
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Non-detection of the effect would a
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system of units to another rather t
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is not SC, and is composed of norma
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the rest of the SC). This would sho
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cylinder has its long axis oriented
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(24) s = Iω where ω is the spin a
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established. For ease of experiment
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lowered into the chamber, alternati
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T < Tc n n T > Tc n 0 Table 1: Inte
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a gravitational BCS type theory is
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III Gravitational London Equations
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VI Conclusion More significant than
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UTF-367/96 Jan 1996 arXiv:supr-con/
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case). To sketch our model - althou
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The constants k and λ are related
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UTF-368/96 Jan 1996 Role of a ”Lo
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mention its scale behaviour and two
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average out. If µ denotes the ener
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We expect that when the Montecarlo
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interact between themselves and pos
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the system can be expressed as E =
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〈( ∑ i ( ∑ i = s ij1 ) 2 +
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as due to the periodic boundary con
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[1] M.J.G. Veltman, in Methods in f
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J. Phys.: Condens. Matter 8 (1996)
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Letter to the Editor L447 Figure 2.
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Letter to the Editor L453 Kato R, E
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The behavior of a Bose condensate -
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indices of the field must be effect
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purely gravitational cosmological t
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(Note that for solutions of (12) on
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effects can arise. Both characteris
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density, there will be a thin layer
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“Mettler 300” scale (300 g full
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any work on it and thus does not fe
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[13] H.W. Hamber and R.M. Williams,
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Appendix: earlier setup. Our first
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FIGURE CAPTIONS 1. Typical double-w
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6. Detection system for the demonst
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Engineering Analysis of the Podklet
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Magnetic Flux Lines around 1/2 of t
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From a Relativistic Phenomenology o
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1. Introduction In this paper we pr
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(Rubin 1993). In fact, throughout t
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Lastly, if we consider a theory of
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3. The Lie conformal pseudogroup as
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ρ s σ(X, Y ) = ρ ic (X, Y ) −
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and ˆf ˆρ = ˆρ. (17) In the la
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Thus, at the sheafs level, the non-
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that µ may be considered as an Abr
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Definition 2 We define the r-th Spe
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Finally, we also have [D 1 , D 2 ]
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4. The potentials of interaction an
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where i Y is the interior product b
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such as ∀ξ k+1 , η k+1 ∈ J k+
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5.2. The gravitational and electrom
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This might be (?) an illustration o
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One uses a rather classical method
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⎧ ⎪⎨ φ µ (α) = − 1 µ,k
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ther their real parts, nor their im
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evolution. In some ways as G. Deleu
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Pommaret, J.-F. 1995 Suites Differe
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2 Introduction The discovery of sup
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4 depressed by a magnetic field [12
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6 symmetry for the cuprates. Surpri
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8 metallic ρ(Τ) α T n with n > 1
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10 pseudogap, two dimensional (2D)
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12 the hole-doped and electron-dope
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14 An example of recent progress in
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16 crystals of these materials [104
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18 Acknowledgments Assistance in pr
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20 [22] M. T. Béal-Monod and K. Ma
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22 [59] A. V. Puchkov, P. Fournier,
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24 [94] A. G. Sun, A. Truscott, A.
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26 Table caption Table 1. (a) Some
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28 Fig. 8. Schematic phase diagram
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30 Table 1. (a) Some important clas
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wave (7). A background discussion o
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Gravitation shielding properties of
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A combination of two different crys
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Full Text Options Access Electronic
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the gravitational ®eld by means of
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ScienceDirect - Technol Rep Tohoku
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New Scientist The World's No.1 Scie
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New Scientist The World's No.1 Scie
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New Scientist---Antigravity *See up
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unaffected by an inch-thick steel p
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Polarizable-Vacuum (PV) representat
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A. Velocity of Light in a Vacuum of
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From the reciprocal of Eq. (10) we
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III. CLASSICAL EXPERIMENTAL TESTS O
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⎡ v L ≈ c ⎢ 1 − 2GM 1 ⎣
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d 2 u dθ + u = GMm 2 O e 2GMu c2 +
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IV. COUPLED MATTER-FIELD EQUATIONS
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B. General Matter-Field Equations
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or 2 GM rc 2 K = e = GM rc 2 K = e
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Comparison of Eqns. (70) - (71) wit
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Table Metric Effects in the Polariz
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16. H. Goldstein, Classical Mechani
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Tony Robertson, Staff Engineer for
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compensation, but with mandatory in
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Emerging Possibilities for Space Pr
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Electrogravitics Systems: An examin
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ELECTROGRAVITICS SYSTEMS REPORTS ON
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CONTENTS Foreword 4 Elizabeth Rausc
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Accelerator Center, Stanford, CA wi
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Introduction, as well as copies of
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ELECTROGRAVITICS SYSTEMS An examina
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DISCUSSION Electrogravitics might b
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particles - that is to say those th
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interrelationship is a difficulty a
Page 869 and 870: electrogravitics. This is one line
Page 871 and 872: In 1955 the number of technicians e
Page 873 and 874: existence and collisions that give
Page 875 and 876: and counterbary. Counterbary is the
Page 877 and 878: ANTI-GRAVITATION RESEARCH The basic
Page 879 and 880: towards realization of a manned veh
Page 881 and 882: ELECTRO-GRAVITIC PROPULSION SITUATI
Page 883 and 884: investment is likely to be necessar
Page 885 and 886: to its present pitch. Beyond the th
Page 887 and 888: ELECTRO-GRAVITICS EFFORT WIDENING C
Page 889 and 890: ELECTROSTATIC MOTORS 40
Page 891 and 892: THE GRAVITICS SITUATION December 19
Page 893 and 894: that no new breakthroughs are neede
Page 895 and 896: equipotentials can be made less con
Page 897 and 898: laboratory man-hours is necessary o
Page 899 and 900: But aviation business is understand
Page 901 and 902: HI i GLOSSARY Gravithermals: Thermi
Page 903 and 904: Magnetogravitics : Boson Fields: Fe
Page 905 and 906: N. Schein, D.M. Haskin and R.G. Cla
Page 907 and 908: similar and allied forces the two e
Page 909 and 910: This movement is practically linear
Page 911 and 912: an assembly of the gravitator cells
Page 913 and 914: space were suddenly filled with man
Page 915 and 916: and utilizing it in the constructio
Page 917 and 918: APPENDIX ffl GRAVITY EFFECTS The or
Page 919: APPENDIX IV A LINK BETWEEN GRAVITAT
Page 923 and 924: ABSTRACT Based on the asymmetry of
Page 925 and 926: do not favor such transitions, and
Page 927 and 928: THE U.S. ANTIGRAVITY SQUADRON by Pa
Page 929 and 930: Clearly, the overseers of black R &
Page 931 and 932: The saucers made by Brown have no p
Page 933 and 934: supersonic velocities. Also, in his
Page 935 and 936: Figure 5. A version of the flying d
Page 937 and 938: dielectrics are a likely choice for
Page 939 and 940: Figure 7. A side view of the B-2 sh
Page 941 and 942: which provides the electrostatic en
Page 943 and 944: for linearly accelerating negative
Page 945 and 946: Unit, London, February 1956. (Libra
Page 949 and 950: 100
Page 951 and 952: 102
Page 953 and 954: 104
Page 955 and 956: 106
Page 957 and 958: 108
Page 959 and 960: 110
Page 961 and 962: 112
Page 963 and 964: Larry Deavenport is a hobbyist in e
Page 965 and 966: various levels and special notice w
Page 967 and 968: The Antigravity Research of T. Town
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Book Review Electrogravitics System
Page 972:
The Hunt for Zero Point
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THE HUNT FOR ZERO POINT. Copyright
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Author's Note and Acknowledgments N
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Prologue The dust devils swirled ar
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Prologue xi The troops had been par
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Chapter 1 From the heavy-handed sty
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NICK COOK 3 Martin Aircraft Company
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NICK COOK 5 In the course of a deca
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NICK COOK 7 "negative weight"—a r
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NICK COOK 9 process, giving somethi
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NICK COOK 11 also levitate paper cl
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Chapter 2 In 1667, Newton mathemati
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NICK COOK 15 I had no direct eviden
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NICK COOK 17 cupped the receiver, b
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NICK COOK 19 Electrogravitics Syste
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NICK COOK 21 dismiss anything that
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NICK COOK 23 the following year swi
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NICK COOK 25 In this, according to
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NICK COOK 27 "degaussed" the brains
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NICK COOK 29 man responsible for so
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NICK COOK 31 Valone seemed quite un
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NICK COOK 33 model flying saucers b
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NICK COOK 35 trying to put the piec
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NICK COOK 37
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Chapter 4 History doesn't relate th
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NICK COOK 41 something—anything
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NICK COOK 43 Park, Maryland. What w
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NICK COOK 45 integral to most moder
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NICK COOK 47 the most baffling myst
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NICK COOK 49 Lusty files were old a
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NICK COOK 51 In the spring of 1941,
Page 1036 and 1037:
NICK COOK 53 near Breslau under the
Page 1038 and 1039:
NICK COOK 55 flying bomb designed t
Page 1040 and 1041:
NICK COOK 57 his death in November
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NICK COOK 59 had developed a revolu
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NICK COOK 61 If there was any sense
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NICK COOK 63 A year after the war e
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NICK COOK 65 yet kicked in and my b
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NICK COOK 67 microfilmed documentat
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NICK COOK 69 reports made by aircre
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NICK COOK 71
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NICK COOK 73 What had I actually le
Page 1058 and 1059:
NICK COOK 75 contract with the Avro
Page 1060 and 1061:
NICK COOK 77 been built, but flight
Page 1062 and 1063:
NICK COOK 79 inaccessible to more t
Page 1064 and 1065:
NICK COOK 81 an antigravity effect
Page 1066 and 1067:
NICK COOK 83 down the aircraft's la
Page 1068 and 1069:
NICK COOK 85 principally to see if
Page 1070 and 1071:
NICK COOK 87 It was then that I rea
Page 1072 and 1073:
NICK COOK 89 started talking about
Page 1074 and 1075:
NICK COOK 91 don't really have a ta
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Chapter 9 A larger-than-life depict
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NICK COOK 95 But ASTP did not end t
Page 1080 and 1081:
NICK COOK 97 questions churned, as
Page 1082 and 1083:
NICK COOK 99 He paused and rubbed t
Page 1084 and 1085:
NICK COOK 101 propulsive antigravit
Page 1086 and 1087:
NICK COOK 103 down. He was abandone
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NICK COOK 105 * * * On the flight d
Page 1090 and 1091:
NICK COOK 107 reaction to the Podkl
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NICK COOK 109 Cleveland and, believ
Page 1094 and 1095:
NICK COOK 111 These vibrating field
Page 1096 and 1097:
NICK COOK 113 Union, using nothing
Page 1098 and 1099:
Chapter 11 If antigravity had been
Page 1100 and 1101:
NICK COOK 117 Stealth had the power
Page 1102 and 1103:
NICK COOK 119 missions in the late
Page 1104 and 1105:
NICK COOK 121 disclosure, however,
Page 1106 and 1107:
Chapter 12 I'd been aware of rumors
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NICK COOK 125 Fellow of the Royal A
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NICK COOK 127 accurate total budget
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NICK COOK 129 F-l 17 A, composed of
Page 1114 and 1115:
Below: Alleged photograph of Rudolp
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Left: John Frost. Below: A cutaway
Page 1118 and 1119:
Above: British Aerospace's concept
Page 1120 and 1121:
Above: The Northrop Grumman B-2 Ste
Page 1122 and 1123:
Above: Map showing key California-b
Page 1125 and 1126:
Below: SS General Hans Kammler - th
Page 1127 and 1128:
Left: Bob Widmer, chief designer of
Page 1129 and 1130:
Metal ingots 'disrupted' by the Hut
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132 The Hunt for Zero Point could s
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134 The Hunt for Zero Point impossi
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136 The Hunt for Zero Point Lockhee
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138 The Hunt for Zero Point The man
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140 The Hunt for Zero Point deduced
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142 The Hunt for Zero Point Brown's
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144 The Hunt for Zero Point Soviet
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Chapter 14 There were two final way
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148 The Hunt for Zero Point all our
Page 1149 and 1150:
150 The Hunt for Zero Point encoura
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152 The Hunt for Zero Point Just as
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154 The Hunt for Zero Point the A-4
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156 The Hunt for Zero Point done an
Page 1157 and 1158:
158 The Hunt for Zero Point as offe
Page 1159 and 1160:
Chapter 16 According to Agoston, Ka
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162 The Hunt for Zero Point not, th
Page 1163 and 1164:
164 The Hunt for Zero Point from Ka
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166 The Hunt for Zero Point mountai
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168 The Hunt for Zero Point service
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Chapter 17 I entered the complex fr
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172 The Hunt for Zero Point had spa
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174 The Hunt for Zero Point signed
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176 The Hunt for Zero Point and int
Page 1177 and 1178:
178 The Hunt for Zero Point have ig
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180 The Hunt for Zero Point radiati
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182 The Hunt for Zero Point to use
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184 The Hunt for Zero Point "And th
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186 The Hunt for Zero Point activit
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188 The Hunt for Zero Point the rea
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190 The Hunt for Zero Point untimel
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192 The Hunt for Zero Point violet
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194 The Hunt for Zero Point There w
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196 The Hunt for Zero Point Even th
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198 The Hunt for Zero Point That ni
Page 1199 and 1200:
200 The Hunt for Zero Point impenet
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Chapter 21 The next day, I was back
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204 The Hunt for Zero Point Many of
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206 The Hunt for Zero Point appeare
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208 The Hunt for Zero Point One suc
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210 The Hunt for Zero Point natural
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212 The Hunt for Zero Point
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214 The Hunt for Zero Point notion,
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216 The Hunt for Zero Point is busi
Page 1217 and 1218:
218 The Hunt for Zero Point during
Page 1219 and 1220:
220 The Hunt for Zero Point Via Sch
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222 The Hunt for Zero Point compres
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224 The Hunt for Zero Point detaile
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226 The Hunt for Zero Point U.S. si
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228 The Hunt for Zero Point the bes
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Chapter 23 Viewed from the back of
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232 The Hunt for Zero Point The ide
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234 The Hunt for Zero Point It was
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236 The Hunt for Zero Point spin-of
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238 The Hunt for Zero Point metal p
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240 The Hunt for Zero Point Martin,
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Chapter 24 The flight was several h
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244 The Hunt for Zero Point morning
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246 The Hunt for Zero Point I was i
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248 The Hunt for Zero Point was one
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250 The Hunt for Zero Point not, as
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252 The Hunt for Zero Point science
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254 The Hunt for Zero Point confirm
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256 The Hunt for Zero Point Einstei
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258 The Hunt for Zero Point had bel
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260 The Hunt for Zero Point theory
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262 The Hunt for Zero Point Hutchis
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264 The Hunt for Zero Point later,
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266 The Hunt for Zero Point Hutchis
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268 The Hunt for Zero Point objects
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270 The Hunt for Zero Point "When y
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272 The Hunt for Zero Point I could
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274 The Hunt for Zero Point that wo
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276 The Hunt for Zero Point orbitin
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278 The Hunt for Zero Point enough
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280 The Hunt for Zero Point Lucas,
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Index Page numbers of illustrations
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284 Index Brown, Thomas Townsend (c
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286 Index Gunston, Bill, 124-25 Gyr
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288 Index NASA (cont'd) Marshall Sp
Page 1289 and 1290:
290 Index Tesla, Nikola, 258-60 Tun
Page 1291:
ABOUT THE AUTHOR Nick Cook is the A
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